Polarization waves and superradiance

Vladimir V. Zheleznyakov, Vit V Kocharovskiĭ, Vlad V Kocharovskiĭ

L. I. Men’shikov

Rostislav M. Arkhipov, A. V. Pakhomov, Mikhail V. Arkhipov +1 more

Using the numerical solution of the system of equations for the amplitudes of bound states, together with the wave equation, we theoretically consider stopped polarization pulse superradiance upon excitation by a pair of half-period attosecond pulses in a thin layer of a five-level resonant medium, the parameters of which are the same as in a hydrogen atom. It is shown that in the case of a multilevel medium, at certain parameters of the exciting field, the superradiance pulse near the medium is also a single-cycle pulse, the shape of which is determined by the first time derivative of the stopped polarization pulse, as in the case when approximate low-level and classical models were used to describe the response of the medium. Keywords: superradiance, attosecond pulses, stopped polarization pulse, unipolar pulses, subcycle pulses.

Yu. A. Avetisyan

The investigation of extended sample superradiance was performed by numerical solution of the semiclassical Maxwell-Bloch equations without using approximation of slowly varying (in space) amplitudes of electric field and medium polarization. The correlations of counter-propagating waves delay times and maximal intensities were analyzed.

Jeng-Yih Su

Rostislav M. Arkhipov, A. V. Pakhomov, Mikhail V. Arkhipov +1 more

Abstract Using the numerical solution of the system of equations for the amplitudes of bound states, together with the wave equation, we theoretically consider stopped polarization pulse superradiance upon excitation by a pair of half-period attosecond pulses in a thin layer of a five-level resonant medium, the parameters of which are the same as in a hydrogen atom. It is shown that in the case of a multilevel medium, at certain parameters of the exciting field, the superradiance pulse near the medium is also a single-cycle pulse, the shape of which is determined by the first time derivative of the stopped polarization pulse, as in the case when approximate low-level and classical models were used to describe the response of the medium.